The general structure of relativistic QFTs

In summary, the conversation discusses the concept of "locality" in quantum physics, specifically in the context of relativistic quantum field theories (QFTs). It is pointed out that the only successful realization of relativistic QFTs is through local interactions, which are necessary to ensure Poincare covariance and the cluster-decomposition principle. The spin-statistics theorem is also mentioned, which states that fields with half-integer spin must be quantized as fermions, while those with integer spin must be quantized as bosons. This local formulation of QFT is able to describe all known particles and their interactions with high precision. Additionally, it is shown that this formulation allows for the existence of entangled states and long-range correlations,
  • #71
I completely agree with @vanhees71 point of view in comment #70. On ‘mathpages.com’ one reads, for example, the following:

People sometimes think that the lack of separability implies ‘action at a distance’, but that's a misunderstanding. Everyone agrees that quantum mechanics does not entail any action at a distance, because no information or energy propagates faster than light. Nevertheless, the entangled parts of a quantum system are not separable, and this is precisely what the violations of Bell's inequality demonstrate. It’s true that in the classical context the only way things could not be separable would be by action at a distance, but the peculiar feature of quantum mechanics is that things can be non-separable without implying any action at a distance. The non-separability is subtle, but it represents a profoundly non-classical aspect of the world.

Entry: “Quantum Mechanics and Separability” (https://www.mathpages.com/home/kmath731/kmath731.htm)
 
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  • #72
Lord Jestocost said:
I completely agree with @vanhees71 point of view in comment #70. On ‘mathpages.com’ one reads, for example, the following:

People sometimes think that the lack of separability implies ‘action at a distance’, but that's a misunderstanding. Everyone agrees that quantum mechanics does not entail any action at a distance, because no information or energy propagates faster than light. Nevertheless, the entangled parts of a quantum system are not separable, and this is precisely what the violations of Bell's inequality demonstrate. It’s true that in the classical context the only way things could not be separable would be by action at a distance, but the peculiar feature of quantum mechanics is that things can be non-separable without implying any action at a distance. The non-separability is subtle, but it represents a profoundly non-classical aspect of the world.

Entry: “Quantum Mechanics and Separability” (https://www.mathpages.com/home/kmath731/kmath731.htm)
I think this is the main reason for the endless discussions. Not whether QM is local or not, but the insistence that "quantum nonlocality" implies some sort of action/interaction/influence and so on at a distance.
 
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  • #73
vanhees71 said:
True, but it's not due to a violation of locality but of "reality", i.e., the concept that all observables take determined values, which are only unknown to us in full detail, so that we describe them statistically, i.e., via probability distributions of some hidden variable(s). That's of course what is not fulfilled according to any QT, including local relativistic QFT. Of course, I use the physical notion of "locality" in the sense of standard relativistic QFTs.
This is way too subtle for most experts to note the subtle difference, imo. Even when they claim that quantum systems don't have definite values at all times, they go on and act and argue as if they had forgotten what they have claimed earlier.
Classicaility is just too overwhelming as a concept to remove completely from thought.
 
  • #74
vanhees71 said:
To describe the coincidence experiments when measuring photon polarization states on different places you need, of course, the two-point correlation (two-photon Green's) function of the (electromagnetic) field. Of course, it's all about correlations. What else?
One cannot arrive at observable consequences of QFT without using Born's rule in one form or another. But Born's rule breaks locality (in the sense of physical continuity between "cause" and "effect"). In its most spectacular applications QFT involves products of local operators at widely separated points in space and time, and applying Born's rule is then a decidedly non-local operation. There is a vestige of continuity in the fields and the operators that describe them, but this continuity applies only to statistical ensembles. Bell's theorem precludes any kind of causal continuity in the individual system.

We share a distaste for quibbling about mere words, and I don't think that our views of QFT are radically different. But I think calling QFT "causally local" causes misperceptions. The epithet "local" applies only to its "deterministic" side. Insisting on locality you are ignoring the vital stochastic (statistical) part of QFT.
 
  • #75
Lord Jestocost said:
I completely agree with @vanhees71 point of view in comment #70. On ‘mathpages.com’ one reads, for example, the following:

People sometimes think that the lack of separability implies ‘action at a distance’, but that's a misunderstanding. Everyone agrees that quantum mechanics does not entail any action at a distance, because no information or energy propagates faster than light. Nevertheless, the entangled parts of a quantum system are not separable, and this is precisely what the violations of Bell's inequality demonstrate. It’s true that in the classical context the only way things could not be separable would be by action at a distance, but the peculiar feature of quantum mechanics is that things can be non-separable without implying any action at a distance. The non-separability is subtle, but it represents a profoundly non-classical aspect of the world.

Entry: “Quantum Mechanics and Separability” (https://www.mathpages.com/home/kmath731/kmath731.htm)
Also from there
Now, it’s well known that no energy or information propagates faster than light according to quantum mechanics, and yet some people still have the vague idea that quantum entanglement implies action at a distance. This may be partly due to lack of clarity about the technical meaning of the word “action” in physics, but also partly due to the fact that the non-separability of quantum mechanics is subtle, involving distant correlations but not communication. People often use sloppy language, saying things like “one electron is affected by the measurement of the other”, but they are really referring to the existence of correlations, not to any action at a distance. Even Bell himself, who evidently yearned for a return to a Lorentzian world view, admitted that instantaneous action at a distance is inconsistent with the well-established Lorentz invariance.
 
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  • #76
WernerQH said:
One cannot arrive at observable consequences of QFT without using Born's rule in one form or another. But Born's rule breaks locality (in the sense of physical continuity between "cause" and "effect"). In its most spectacular applications QFT involves products of local operators at widely separated points in space and time, and applying Born's rule is then a decidedly non-local operation. There is a vestige of continuity in the fields and the operators that describe them, but this continuity applies only to statistical ensembles. Bell's theorem precludes any kind of causal continuity in the individual system.

We share a distaste for quibbling about mere words, and I don't think that our views of QFT are radically different. But I think calling QFT "causally local" causes misperceptions. The epithet "local" applies only to its "deterministic" side. Insisting on locality you are ignoring the vital stochastic (statistical) part of QFT.
It's correlations, not causal effects, that's described by the correlation functions. That's the important point of the whole debate! You evaluate the joint probability for registering a photon pair at two space-like separated events. This has nothing to do with non-local interactions.
 
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  • #77
vanhees71 said:
It's correlations, not causal effects, that's described by the correlation functions.
How do correlations arise, if not through causal effects?
 
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  • #78
vanhees71 said:
it's not due to a violation of locality but of "reality"
Again you are insisting on your preferred definitions of words. Some people use "locality" to mean "the Bell inequalities are not violated". Certainly that is the usage implied by item (1) in the post that I responded to. I understand you don't like this usage, but that's beside the point. Not everyone uses words the way you would like them to be used.

vanhees71 said:
It is, in my opinion, mandatory to use "inseparable" rather than "nonlocal", because locality and thus also its negation have a precise mathematical meaning in relativistic local (sic!) QFTs,
In my opinion, as I've already stated, we should stop using vague ordinary language words altogether. "Inseparable" is vague ordinary language; that word can have multiple meanings, just like "locality". Instead of saying "inseparable", state the precise mathematical condition you are referring to (just like saying "spacelike separated measurements commute" instead of "locality"). Then we all know what we are talking about and we can stop having pointless arguments over words and discuss physics instead.
 
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  • #79
Do I have to follow your opinion that I should not use the standard meaning of words and instead use some imprecise and confusing language? What should this be good for? Is PF now a philosophy forum rather than a physics forum? That'd be a pity...
 
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  • #80
vanhees71 said:
Do I have to follow your opinion that I should not use the standard meaning of words
The whole point is that there is not a single "standard meaning" for the words that are creating these problems. I have said this again and again and you continue to ignore it.

vanhees71 said:
and instead use some imprecise and confusing language?
I said no such thing. I said you should explicitly give the precise mathematical condition you are using instead of using imprecise and confusing language. For example, instead of saying "inseparable" you should say the precise mathematical condition that you are referring to with that word.
 
  • #81
I did this repeatedly. It's impossible to get any further if one only repeats the same well-known definitions again and again.
 
  • #82
vanhees71 said:
I did this repeatedly.
Where have you given the precise mathematical condition that you are using the term "inseparable" to refer to?
 
  • #83
vanhees71 said:
It's impossible to get any further if one only repeats the same well-known definitions again and again.
You are missing the point. Nobody has ever disputed the fact that QFT has the mathematical property you say it has (that spacelike separated measurements commute).

However, the argument you continue to insist on making is that QFT is "local" because it has that mathematical property. That argument is nonsense as an argument; it's a definition of the term "local", not an argument for why QFT is "local". And it's also a pointless argument, since what we are supposed to be discussing is the physics, not the definitions of words.
 
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  • #84
Then you should finally tell me what you think the word "local" means in the context of relativistic QFT. I use the word in the standard sense used in all modern textbooks about the subject, and I've summarized it in #1 of this thread. The details fill the first few chapters of Weinbergs QT of fields vol. 1. It's impossible to understand and communicate about an exact science, if it is not allowed to use the standard definitions and terminology of the vast majority of the science community. You are also usually a proponent of this rule for PF. So I'm very surprised that particularly you are fighting my attempt to clarify this confusion by pointing to the standard meaning of the word "locality".

BTW: A bipartite quantum system is called separable, if it's state can be written in the form
$$\hat{\rho}=\sum_j p_j \hat{\rho}_j^{(A)} \otimes \hat{\rho}_j^{(B)}$$
with ##p_j>0## and ##\sum_j p_j=1##.
 
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  • #85
vanhees71 said:
Then you should finally tell me what you think the word "local" means in the context of relativistic QFT.
I have already done that in multiple posts, but I'll summarize again here. The "relativistic QFT" one is "spacelike separated measurements commute", which is the definition you've been using. The other one I've referred to multiple times is "the Bell inequalities are not violated". Bell's original paper got more specific about the latter and used "locality" to describe the factorizability condition on the joint probability distribution for measurement results (equation 2 in his original paper).

vanhees71 said:
It's impossible to understand and communicate about an exact science, if it is not allowed to use the standard definitions and terminology of the vast majority of the science community.
The "relativistic QFT" community is not the same as "the vast majority of the science community". It would be very nice if the entire "science community" agreed on one definition for the word "locality". But it hasn't. The fact that you only recognize one definition as "standard" does not mean all your beliefs about that definition are correct.

vanhees71 said:
A bipartite quantum system is called separable, if it's state can be written in the form
$$\hat{\rho}=\sum_j p_j \hat{\rho}_j^{(A)} \otimes \hat{\rho}_j^{(B)}$$
with ##p_j>0## and ##\sum_j p_j=1##.
Is this equivalent to saying that a "separable" system is not entangled, and vice versa?
 
  • #86
vanhees71 said:
You are also usually a proponent of this rule for PF. So I'm very surprised that particularly you are fighting my attempt to clarify this confusion by pointing to the standard meaning of the word "locality".
Your repeated posts have not clarified any confusion, because nobody is confused about the actual physics involved. All your repeated posts have done is caused pointless arguments because other posters here, including ones with considerable knowledge of the subject matter under discussion, do not use the word "locality" the same way you do and object to your talking as if your preferred usage was the only one that exists.
 
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  • #88
This thread can remain closed. I think we've beat this topic to death (at least for the time being). This thread demonstrates that the meaning of "local" is context-dependent. To avoid wheel spinning over terminology. it behooves us to be explicit about what we mean when using the term.
 
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